A light emitting device including a waveguide having an electrically pumped gain region, a saturable absorber, a nonlinear crystal, an inclined mirror, and a light-concentrating structure. Light pulses emitted from the gain region are reflected by the inclined mirror and focused by the light-concentrating structure into the nonlinear crystal in order to generate frequency-converted light pulses. The gain region, the saturable absorber, the light-concentrating structure and the inclined mirror are implemented on or in a common substrate. The resulting structure is stable and compact, and allows on-wafer testing of produced emitters. The folded structure allows easy alignment of the nonlinear crystal.
Legal claims defining the scope of protection, as filed with the USPTO.
1. A light emitting device, comprising: a waveguide having an electrically pumped gain region; a saturable absorber; a coupling structure; a light-concentrating structure; a substrate; and a nonlinear medium; wherein said saturable absorber and said gain region are adapted to emit first light pulses, said coupling structure together with said light-concentrating structure being adapted to couple said first light pulses into said nonlinear medium, said nonlinear medium being adapted to generate second light pulses such that an optical frequency of said second light pulses is higher than an optical frequency of said first light pulses; said gain region, said saturable absorber, said coupling structure, and said light-concentrating structure being implemented on or in said substrate such that said coupling structure is adapted to change a direction of said first light pulses by an angle which is in the range of 70 to 110 degrees.
2. The device according to claim 1 , wherein an individual pulse of said first light pulses has a first photon and a second photon, the optical frequency of a photon of a generated second light pulse being equal to the sum of an optical frequency of the first photon and an optical frequency of the second photon.
3. The device according to claim 1 , wherein the optical frequency of said second light pulses is equal to two times the optical frequency of said first light pulses.
4. The device according to claim 1 , further comprising: a partially reflecting structure to define an optical cavity together with a back reflector, said optical cavity comprising said gain region.
5. The device according to claim 4 , wherein said partially reflecting structure comprises a frequency-selective structure.
6. The device according to claim 5 , wherein said optical cavity comprises only one frequency-selective structure which has a reflection bandwidth narrower than or equal to 5 nm.
7. The device according to claim 1 , wherein said nonlinear medium comprises a nonlinear crystal comprising a frequency-selective structure to provide feedback to said gain region.
8. The device according to claim 7 , wherein said frequency-selective structure is arranged to provide feedback through said nonlinear crystal to said gain region.
9. The device according to claim 7 wherein said frequency-selective structure comprises a Bragg grating implemented in or on said nonlinear crystal.
10. The device according to claim 5 , further comprising: a distributed Bragg reflector which is located between said coupling structure and said nonlinear medium.
11. The device according to claim 1 , further comprising: a plurality of substantially parallel waveguides to emit said first light pulses, the first light pulses emitted by said plurality of waveguides being coupled into a single nonlinear crystal.
12. The device according to claim 1 , wherein said light-concentrating structure comprises a curved surface adapted to collimate or focus light into said nonlinear material.
13. The device according to claim 12 , wherein said substrate comprises a curved surface.
14. The device according to claim 1 , wherein said light-concentrating structure comprises a diffractive structure.
15. The device according to claim 1 , further comprising: a further waveguide to confine light of said first light pulses, said further waveguide comprising said nonlinear medium.
16. The device according to claim 15 , wherein said further waveguide comprises a tapered portion to concentrate light into a narrow part of said further waveguide.
17. The device according to claim 15 , wherein said non-linear medium is a crystal having one or more convex facets to refract said first light pulses into said further waveguide.
18. The device according to claim 1 , wherein the first light pulses introduced into said nonlinear medium have a predetermined polarization, and said nonlinear medium has periodically poled zones to provide quasi phase matching such that said second light pulses are in a same phase for each poling period, the orientation of said zones being matched with a polarization of said first light pulses.
19. The device according to claim 18 , further comprising: a polarization-rotating element.
20. The device according to claim 1 , wherein a bias voltage of said gain region and a bias voltage of said saturable absorber are separately controllable.
21. A method for generating light pulses by using a waveguide comprising an electrically pumped gain region, a saturable absorber, a coupling structure, a substrate, a light-concentrating structure, and a nonlinear medium, said gain region, said saturable absorber, said coupling structure, and said light-concentrating structure being implemented on or in said substrate, said method comprising: providing first light pulses using said saturable absorber and said gain region; changing the direction of said first light pulses by an angle which is in the range of 70 to 110 degrees by said coupling structure; and focusing or collimating said first light pulses by said light-concentrating structure into said nonlinear medium in order to generate second light pulses such that an optical frequency of said second light pulses is higher than an optical frequency of said first light pulses.
22. The method according to claim 21 , wherein a first light pulse comprises a first photon and a second photon, the optical frequency of a photon of a generated second light pulse is equal to the sum of an optical frequency of the first photon and an optical frequency of the second photon.
23. The method according to claim 21 , wherein the optical frequency of said second light pulses is equal to two times the optical frequency of said first light pulses.
24. The method according to claim 21 , further comprising: changing the bias voltage of said saturable absorber between a first voltage level and a second voltage level.
25. A projecting device, comprising: projecting optics; and a light emitting device, said light-emitting device in turn comprising: a waveguide having an electrically pumped gain region, a saturable absorber, a coupling structure, a light-concentrating structure, a substrate, and a nonlinear medium, wherein said saturable absorber and said gain region are adapted to emit first light pulses, said coupling structure together with said light-concentrating structure being adapted to couple said first light pulses into said nonlinear medium, wherein said nonlinear medium is adapted to generate second light pulses such that an optical frequency of said second light pulses is higher than an optical frequency of said first light pulses, wherein said gain region, said saturable absorber, said coupling structure, and said light-concentrating structure are implemented on or in said substrate such that said coupling structure is adapted to change the direction of said first light pulses by an angle which is in the range of 70 to 110 degrees.
26. The projecting device according to claim 25 , further comprising: a two-dimensional modulator array.
27. The projecting device according to claim 25 , further comprising: at least one beam directing device, wherein said first light pulses are adapted to be generated by semi-passive Q-switching.
Cooperative Patent Classification codes for this invention. Click any code to explore related patents in that topic.
January 17, 2008
May 17, 2011
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